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Polyphenylene model

Figure 3.4. The polyphenylene model based on the concepts of Gibson et al. (1946) and... Figure 3.4. The polyphenylene model based on the concepts of Gibson et al. (1946) and...
Scheme 20. Polyphenylene dendrimers in the 1st 68 and in the 2nd generation 70 which are decorated with fluorescent perylene imide chromophores on the surface. Perylenedicarboxi-mide derivative 69 serves as a model compound for spectroscopic investigations. Scheme 20. Polyphenylene dendrimers in the 1st 68 and in the 2nd generation 70 which are decorated with fluorescent perylene imide chromophores on the surface. Perylenedicarboxi-mide derivative 69 serves as a model compound for spectroscopic investigations.
Scheme 9. Three-dimensional stick-and-ball model of the first four generations of a polyphenylene dendrimer built from the biphenyl core and the A2B building blocks... Scheme 9. Three-dimensional stick-and-ball model of the first four generations of a polyphenylene dendrimer built from the biphenyl core and the A2B building blocks...
Confocal fluorescence microscopy images in a polymer film of a second-generation polyphenylene dendrimer with eight perylenemonoimide functions at the periphery 49 and a model compound bearing one single perylenemonoimide 50 reveal that the dendrimer exhibits a three- to fourfold intensity and an obvious blinking in comparison to the model compound which shows only uniform spots with less dynamics (Scheme 19) [69]. [Pg.30]

The deficiency of this model is the assumption of only light doping. However the soliton conductivity has also been established in highly doped material and not only for polyacetylene, but for polyphenylene too, in which the solitons cannot exist... [Pg.32]

In general, doping tends to lead to a loss of x-ray order in polyacetylene and polyphenylene, suggesting that dopant ions may be distributed more or less at random. The structural models shown in Fig. 16 are clearly idealised as only limited order is seen even in cation-doped polymer. The anion dopants are much larger and apparently disrupt the structure too much for any sign of regularity to be seen, except in the case of iodine. [Pg.66]

FIGURE 9.4 Dependence of constants (a, b, and c present Henry constant, sorption affinity constant, and Langmuir sorption capacity respectively) of the model of dual-mode sorption of hydrocarbons by glassy polyphenylene oxides on boiling temperatures of hydrocarbons Z), is pDMePO, poly-2,6-dimethyl-l,4-phenylene oxide o is pDPhPO, poly-2,6-diphenyl-l,4-phenylene oxide is pDMePO/pDPhPO copolymer (97.5/2.5% mol) v is pDMePO/pDPhPO copolymer (75/25% mol). (From analysis of results presented in Lapkin, A.A., Roschupkina, O.P., and Ilinitch, O.M., J. Membr. Sci., 141, 223, 1998.)... [Pg.237]

Permeability and diffusion coefficients of hydrocarbons in polyphenylene oxides are also essentially dependent on pressure (see Figure 9.23). It can be seen that in the case of ethylene, with the increase in pressure, the permeability coefficients first decrease, and then begin to rise. Ref. [18] quotes constants of the dual-mode sorption model for a number of hydrocarbons permeation through polyphenylene oxide. [Pg.255]

The origin of the conduction mechanism has been a source of controversy ever since conducting polymers were first discovered. At first, doping was assumed to simply remove electrons from the top of the valence band (oxidation) or add electrons to the bottom of the conduction band (reduction). This model associates charge carriers with free spins (unpaired electrons). However, the measured conductivity in doped polyacetylene (and other conducting polymers such as polyphenylene and polypyrrole) is r greater than what can be accounted for on the basis of free spin alone. [Pg.32]

Fig. 14. (a) Solid-state l3C spinning sideband patterns (sum projections) for the aromatic ternary CH in polyphenylene dendrimers, obtained at a spinning frequency of vR = 25 kHz. The spectra were recorded for different temperatures and generations, (b) Corresponding simulated spectra, obtained by taking into account different models of phenyl ring reorientation processes on a microsecond-timescale. For details, see ref. 44. [Pg.20]

Fig. 15. (a) Normalized pure-exchange CODEX intensities E(tm) as a function of tm for the aromatic ternary CH and the quaternary Cquat in Td-G2(-Me),6 dendrimer (T=363K). The fit curve for the ternary carbons is a stretched exponential cxp[—(rln/rcyi with /I = 0.51 and tc = 401 ms. The dotted line indicates the final CODEX exchange intensities, (b) Motional model of the localized, cooperative dynamics in polyphenylene dendrimers, including two-site jumps of all phenyl substituents of a pentaphenyl benzene building block. As indicated by X-ray analysis and computer simulations, the peripheral aromatic rings are inclined by 30° with respect to an axis normal to the face of the central benzene ring. For details, see ref. 44. [Pg.21]

Progress has also been made in part cooling. Portable and centralized chillers have been developed to cool the part in a minimum time. These closed loop systems use water or water-ethylene glycol combinations as the heat transfer medium. The application of heat transfer principles allows one to computer model the cooling process (35). For the new engineering resins such as polyamide-imide and polyphenylene sulfide, one must use mold heating. The use... [Pg.599]

Also, the threefold coordination of the Co centers in the dicarbonitrile nanomeshes described above could be rationalized with the help of DFT calculations. For the modeling, the molecular linkers were simplified as NC-Phi-CN refaining the carbonitrile endgroups that interact with the Co centers. In addition, the molecules were confined in a plane in accordance with the STM data, showing that the aromatic polyphenylene linkers are ad-... [Pg.28]

Techniques for chloromethylating polyaiylether sulfones, polyphenylene oxide, phenolic resins, and model compounds were described recently. When the subsequent products are converted... [Pg.426]

FIGURE 8 The X-ray powder diffraction (XRD) patterns of two ferrocene-containing polyphenylene samples FP-6 (b), and FPSC-5 (c) after heating at 250°C, and the model spectra of two iron-based oxides (a). [Pg.83]

Among the polyphenylene-based materials highly emissive PFs have received particular attention due to their extraordinary properties in device applications as originally demonstrated by Bradley [74,76-78]. In addition to the wide variety of synthetic routes allowing for the synthesis of differently substituted homopolymers as well as copolymers, PFs display attractive optical and electronic properties which make them ideal model systems for studying relevant structure to property relations in conjugated polymers as shown by Cadby et al. [77,116]. For this reason different properties which are related to the molecular structure as well as to intrachain order effects of the polymer shall be discussed in the following. [Pg.137]

Techniques for chloromethylating polyarylether sulfones, polyphenylene oxide, phenolic resins, and model compounds were described recently [191]. When the subsequent products are cmiverted to quaternary amines, there is a decrease in the quatemization rate with increase in degree of substitutimi. This may be due to steric effects imposed by restricted rotation of the polymeric chains [191]. This phenomenon was not observed in quatemization of poly(chloromethyl styrene). The chloromethylation reaction of a polysulfone with chloromethyl ether, catalyzed by stannic chloride, can be illustrated as follows ... [Pg.599]

Table 3.14 shows limit values of the optical parameters calculated according to Eqs. 3.41 and 3.42 for systems A, C, E, F, and H shown in Fig. 3.13. Polystilbenes (F) are combinations of model planar polyphenylenes and traus-polyenes. System H can also be represented as a combination of poly-para-quinodimethane and transpolyene. [Pg.87]


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See also in sourсe #XX -- [ Pg.94 ]




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Polyphenylenes

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